JP2015516557A - Magnetic bearing and method for mounting a ferromagnetic structure around an iron core of a magnetic bearing - Google Patents

Abstract

A radial actuator part and an axial actuator part are provided, the radial actuator part comprising a layered stator stack (2) provided with a stator yoke (3), wherein the stator yoke (3) And being linked to a closed ferromagnetic structure (9) surrounding the stator yoke (3). [Selection] Figure 6

Description

  The present invention relates to a magnetic bearing for a rotating machine, where the bearing exhibits an integral radial-axial design and the axial control flux passes through the central opening of the soft magnetic core.

  Magnetic bearings provide contactless suspension. Low friction loss means that magnetic bearings are attractive for high speed applications. However, high speed rotating machine designs are often complex due to the dynamic constraints of the rotor. In this regard, each reduction in axial length contributes to the rotor dynamic limit. This characteristic is maximally applied in “combo bearings”, ie bearings designed to integrate axial and radial channels into a compact configuration sharing various functional components.

  Various examples of combo bearings are described in patents and literature. In many cases, the path of the axial control flux traverses the central hole of the stack of layered ferromagnetic materials. This example is described in patents or patent applications such as Patent Document 1, Patent Document 2, Patent Document 3, Patent Document 4, and Patent Document 5. Other examples are described in publications such as Imberdorf et al., Pichot et al. And Buckner et al. In the type of combo bearing shown in Blumenstock US Pat. No. 6,057,059, the axial control flux does not cross the central hole of the stack of layered ferromagnetic material.

  The performance of the axial channel of the combo bearing is more generally that if the path of the axial control flux traverses the central hole in the stack of laminates, the combo bearing contains a section where the conductive path surrounds the control flux. In some cases, it may be adversely affected. In that case, the changing control magnetic flux generates a voltage in the surrounding material. If the surrounding path is closed and conductive, the generated voltage results in circulating current and consequently Joule loss. In practice, such a stack of laminates can be thought of as a short-circuit secondary winding of a transformer, and the axial control winding is the primary winding. The result depends on the frequency, and in principle, the loss increases as the frequency increases. For a particular axial control current and frequency, Joule loss reduces the force that should be generated. As a result, the performance of the axial channel is affected.

  Similar phenomena can occur in a stack of laminates in which an axial actuator operates. In this case, the control axial flow enters the stack itself, but the physical interpretation remains the same. In Patent Document 2, Takahashi proposes to provide a series of evenly distributed radial cuts in such a stack of laminates. Of course, the laminate is not cut through its entire thickness in order to maintain sufficient strength. As a result, if the control magnetic flux enters only the cut region, the induced current remains locally. This technique offers only a solution for reducing losses in the stack of related laminates. The total control flux is always surrounded by another stator stack.

  U.S. Patent No. 6,057,032 describes a method for removing eddy currents induced in a stator stack by an axial control field. This is accomplished by making cuts through each layer of the stack and stacking the layers so that the magnetic resistance to the magnetic field in the stack is minimized. The disadvantage of this method is the reluctance to the magnetic field caused by the increased radial control winding. Furthermore, as is known, the coating between the layers is not completely insulating, the parts of the assembly can provide contact between the layers, and the circulating current is still observed. Thus, additional means for removing these eddy currents can further improve performance.

US Pat. No. 5,514,924 US Pat. No. 6,268,674 US Pat. No. 6,727,617 International Publication No. 2008/074045 Chinese Patent No. 1,737,388 Specification US Patent 6,359,357 B1 Specification International Publication No. 2011/054065

  The object of the present invention is to provide an alternative method for reducing the losses as a result of eddy currents.

  For this purpose, the present invention is a magnetic bearing, comprising a radial actuator part and an axial actuator part, wherein the radial actuator part is provided with a layered stator stack provided with a stator yoke, The yoke relates to a magnetic bearing linked to a closed ferromagnetic structure surrounding the stator yoke.

  In order to better illustrate the features of the present invention, some preferred embodiments of the magnetic bearing according to the present invention will now be described by way of example and without limitation, with reference to the accompanying drawings.

1 shows a longitudinal section of a known combo bearing. 1 shows a longitudinal section of a known combo bearing. 1 shows a longitudinal section of a known combo bearing. 1 shows a radial cross section of a known combo bearing. 1 shows a radial cross section of a known combo bearing. Fig. 2 schematically shows a perspective view of a part of a magnetic bearing according to the invention that generates a radial force. Fig. 7 shows a section along the line VII-VII in Fig. 6; FIG. 8 shows successive steps in the assembly of the ferromagnetic structure according to FIG. FIG. 8 shows successive steps in the assembly of the ferromagnetic structure according to FIG. 8 shows various embodiments of a yoke of a stack of laminates according to FIG. Fig. 11 shows a part of a ferromagnetic structure according to Fig. 10; FIG. 15 shows an exploded view of the ferromagnetic structure according to FIG. 14. 8 shows various embodiments of a yoke of a stack of laminates according to FIG. 8 shows various embodiments of a yoke of a stack of laminates according to FIG. FIG. 15 shows an exploded view of the ferromagnetic structure according to FIG. 14. FIG. 15 shows an exploded view of the ferromagnetic structure according to FIG. 14.

  Several longitudinal sections of the state of the art combo bearing type are shown in FIGS. Two possible radial cross-sections of the state of the art combo bearing type are shown in FIGS.

  The alternative designs shown all consist of a layered rotor stack 1, a layered stator stack 2, a stator yoke 3, a pole yoke 12, two axial poles 4a and 4b, and at least three radial poles 5.

The axial force is controlled by an axial control winding 6 whose structure is rotationally symmetric.
The radial force is controlled by a radial control winding 7 wound around the radial pole 5.

  When a bias magnetic field is not generated by the permanent magnet 8, the bias current is added to the axial control current by a specific method, or the bias current also shows a rotationally symmetric form and is localized near the axial control winding 6. A bias magnetic field can be generated by guiding through a separate, separate bias winding. The aforementioned bias winding has the same structure as the axial control winding 6, is physically separated from the axial control winding 6, and is in the immediate vicinity of the axial control winding 6.

  When current is applied to the radial control winding 7, magnetic flux begins to flow in the plane of the layers of the stator stack 2.

  The magnetic flux generated by the current applied to the axial control winding 6 flows through the pole yoke 12, then enters the axial pole 4a, crosses the split section, enters the rotor stack 1, and passes the split section. It traverses toward the opposite axial pole 4b and finally returns to the pole yoke 12.

  According to Faraday-Lenz and Ohm's law, circulating current is generated in the layers of the stator stack 2. The object of the present invention is therefore to provide a damping device for this induced circulating current.

  The impedance experienced by the circulating current is mainly determined by the tangential resistance of the layer stack.

  Although there is some inductive contribution, it is relatively limited. The present invention relates to mounting additional devices around a layered stack that generally increases the inductive contribution to impedance.

  According to the invention, this object is achieved in a practical way by a stator yoke linked to a closed ferromagnetic structure 9 surrounding the stator yoke 3 shown in FIG.

  In practice, this “linked” means that, as in the case of two links in a chain linked together, the aforementioned ferromagnetic structure 9 in fact surrounds a part of the stator yoke 3 while the stator The yoke 3 also means surrounding a part of the ferromagnetic structure 9 described above.

  7, 10, 13 and 14 show axial sections of the stator yoke 3 of the stack of laminates, along with some typical variations of the surrounding hollow ferromagnetic structure 9.

  In order to maximize the performance of the method, it is ideal to take additional measures to limit or prevent eddy currents generated in the hollow ferromagnetic structure.

  This is achieved, for example, by assembling the hollow ferromagnetic structure 9 with a component 10 such as a ferrite component, a soft magnetic composite component, or a stacked thin ferromagnetic layer component.

  In order to minimize the magnetoresistance and cost of the ferromagnetic structure, the aforementioned components are preferably U-shaped as shown in FIG.

  FIG. 9 shows how such a U-shaped part can be mounted around the stator yoke 3. Instead of using the U-shaped part 10, a straight part 11 can also be used as shown in FIG.

  FIG. 12 shows how the straight part 11 of FIG. 11 can be mounted around the stator yoke 3. In order to minimize reluctance, the parts need to be pressed together.

  However, such a hollow ferromagnetic structure 9 can also be produced by winding an amorphous ribbon or a nanocrystal ribbon around the stator yoke 3 of the stack of laminated materials as shown in FIG.

  Instead of winding these materials directly, they are wound on separate structures as shown in FIG. 15 and the resulting hollow ferromagnetic structure is divided into several parts, as shown in FIG. The parts can then be rejoined together around the stator yoke 3 of the stack of laminates and the parts can be pressed together to minimize the magnetic resistance.

  The present invention is in no way limited to the embodiments described above and shown in the drawings, and a magnetic bearing according to the present invention can be realized in all kinds of variants without departing from the scope of the present invention. it can.

1: layered rotor stack 2: layered stator stack 3: stator yokes 4a, 4b: axial pole 5: radial pole 6: axial control winding 7: radial control winding 8: permanent magnet 9: closed Type ferromagnetic structure

Claims (15)

A radial bearing portion and an axial actuator portion, the radial actuator portion comprising a layered stator stack (2) provided with a stator yoke (3),
Magnetic bearing, characterized in that the stator yoke (3) is linked to a closed ferromagnetic structure (9) surrounding the stator yoke (3). The axial actuator portion includes at least one axial control coil surrounding the layered stator stack (2), and further includes a pole yoke (12) and two axial poles (4a and 4b),
A permanent magnet (8) is provided between the stator yoke (3) and the two axial poles (4a and 4b);
The permanent magnet (8) is magnetized in the axial direction,
Magnetic bearing according to claim 1, characterized in that the magnetization direction of the permanent magnet (8) is opposite on both axial sides of the stator yoke (3).   A radially magnetized permanent magnet (8) surrounds the layered stator stack (2), and at least one axial control winding (6) of the axial actuator section is connected to the layered stator stack (2). The magnetic bearing according to claim 1, wherein the magnetic bearing is mounted on at least one axial side of the radially magnetized permanent magnet (8).   Magnetic bearing according to claim 3, characterized in that the radially magnetized permanent magnet (8) is configured as a series of adjacently mounted small permanent magnets. The axial actuator portion includes at least one axial control winding (6), a pole yoke (12), and two axial poles (4a and 4b),
Magnetic bearing according to claim 1, characterized in that the at least one axial control winding (6) is mounted on at least one axial side of the layered stator stack (2).   Magnetic bearing according to claim 5, characterized in that the pole yoke (12) contacts the stator yoke (2).   A bias winding having the same configuration as the axial control winding (6), physically spaced from the axial control winding (6) and proximate to the axial control winding (6); The magnetic bearing according to claim 5, wherein the magnetic bearing is provided.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) comprises a stack of thin layers that are electrically insulated from one another.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) comprises a wound flat ribbon.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) contains ferrite.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) comprises a soft magnetic composite powder.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) comprises an amorphous or nanocrystalline material.   Magnetic bearing according to claim 1, characterized in that the closed ferromagnetic structure (9) comprises a number of interconnected parts. A method for manufacturing a magnetic bearing, the method comprising:
-Preparing the stator yoke (3);
Providing a set of ferromagnetic parts forming a closed path having an internal dimension that is greater than or equal to the external dimension of the axial cross section of the stator yoke (3);
Placing the ferromagnetic component around the stator yoke (3) such that a closed path is formed;
-Strongly pressing all the ferromagnetic parts together;
Fixing the resulting ferromagnetic structure (9) to the stator yoke (3);
A method comprising the steps of: A method for manufacturing a magnetic bearing, the method comprising:
-Preparing the stator yoke (3);
Providing a ferromagnetic material on the bobbin, such as an amorphous ribbon, nanocrystalline ribbon, magnetic wire or fiber material;
Electrically insulating the stator yoke (3);
Winding the ferromagnetic material on the bobbin around the stator yoke (3) to form a ferromagnetic structure (9) around the stator yoke (3);
Fixing the resulting ferromagnetic structure (9) to the stator yoke (3);
A method comprising the steps of:

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